{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1993:RTYYYVNMX5OPQWWYQ5N7VUAJQL","short_pith_number":"pith:RTYYYVNM","schema_version":"1.0","canonical_sha256":"8cf18c55acbf5cf85ad8875bfad00982cbb5d02554069ce6bd8e98e66d8cf3cd","source":{"kind":"arxiv","id":"hep-ph/9308279","version":1},"attestation_state":"computed","paper":{"title":"Pseudo-Stable Bubbles","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Marcelo Gleiser","submitted_at":"1993-08-16T17:36:36Z","abstract_excerpt":"The evolution of spherically symmetric unstable scalar field configurations (``bubbles'') is examined for both symmetric (SDWP) and asymmetric (ADWP) double-well potentials. Bubbles with initial static energies $E_0\\la E_{{\\rm crit}}$, where $E_{{\\rm crit}}$ is some critical value, shrink in a time scale determined by their linear dimension, or ``radius''. Bubbles with $E_0\\ga E_{{\\rm crit}}$ evolve into time-dependent, localized configurations which are {\\it very} long-lived compared to characteristic time-scales in the models examined. The stability of these configurations is investigated an"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"hep-ph/9308279","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1993-08-16T17:36:36Z","cross_cats_sorted":[],"title_canon_sha256":"ce8c530447634906580fc77da4c60ae599c15d1987841e9a85ee4d7298b44ae0","abstract_canon_sha256":"7978c7e4b9b2a227e672b1adffe2693a19df7ab13626a60477150e551e7e5444"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:55:50.290592Z","signature_b64":"SzY3WEQ9kW8Tf4Ai2TSDcf6yiEp5TU2UjLLIi4NeAyK+iOqPuo1s894tuq6NyPqzvyAYyYx3620d1ZszuMN3DQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8cf18c55acbf5cf85ad8875bfad00982cbb5d02554069ce6bd8e98e66d8cf3cd","last_reissued_at":"2026-07-04T15:55:50.290244Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:55:50.290244Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Pseudo-Stable Bubbles","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Marcelo Gleiser","submitted_at":"1993-08-16T17:36:36Z","abstract_excerpt":"The evolution of spherically symmetric unstable scalar field configurations (``bubbles'') is examined for both symmetric (SDWP) and asymmetric (ADWP) double-well potentials. Bubbles with initial static energies $E_0\\la E_{{\\rm crit}}$, where $E_{{\\rm crit}}$ is some critical value, shrink in a time scale determined by their linear dimension, or ``radius''. Bubbles with $E_0\\ga E_{{\\rm crit}}$ evolve into time-dependent, localized configurations which are {\\it very} long-lived compared to characteristic time-scales in the models examined. The stability of these configurations is investigated an"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9308279","kind":"arxiv","version":1},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/hep-ph/9308279/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/9308279","created_at":"2026-07-04T15:55:50.290307+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9308279v1","created_at":"2026-07-04T15:55:50.290307+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9308279","created_at":"2026-07-04T15:55:50.290307+00:00"},{"alias_kind":"pith_short_12","alias_value":"RTYYYVNMX5OP","created_at":"2026-07-04T15:55:50.290307+00:00"},{"alias_kind":"pith_short_16","alias_value":"RTYYYVNMX5OPQWWY","created_at":"2026-07-04T15:55:50.290307+00:00"},{"alias_kind":"pith_short_8","alias_value":"RTYYYVNM","created_at":"2026-07-04T15:55:50.290307+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2606.22680","citing_title":"Unified theory of oscillons and modes","ref_index":3,"is_internal_anchor":true},{"citing_arxiv_id":"2604.26795","citing_title":"A positive definite formulation of vacuum decay with reduced symmetry","ref_index":25,"is_internal_anchor":false},{"citing_arxiv_id":"2604.04494","citing_title":"Multi-field oscillons/I-balls in the Friedberg-Lee-Sirlin model","ref_index":10,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/RTYYYVNMX5OPQWWYQ5N7VUAJQL","json":"https://pith.science/pith/RTYYYVNMX5OPQWWYQ5N7VUAJQL.json","graph_json":"https://pith.science/api/pith-number/RTYYYVNMX5OPQWWYQ5N7VUAJQL/graph.json","events_json":"https://pith.science/api/pith-number/RTYYYVNMX5OPQWWYQ5N7VUAJQL/events.json","paper":"https://pith.science/paper/RTYYYVNM"},"agent_actions":{"view_html":"https://pith.science/pith/RTYYYVNMX5OPQWWYQ5N7VUAJQL","download_json":"https://pith.science/pith/RTYYYVNMX5OPQWWYQ5N7VUAJQL.json","view_paper":"https://pith.science/paper/RTYYYVNM","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/9308279&json=true","fetch_graph":"https://pith.science/api/pith-number/RTYYYVNMX5OPQWWYQ5N7VUAJQL/graph.json","fetch_events":"https://pith.science/api/pith-number/RTYYYVNMX5OPQWWYQ5N7VUAJQL/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/RTYYYVNMX5OPQWWYQ5N7VUAJQL/action/timestamp_anchor","attest_storage":"https://pith.science/pith/RTYYYVNMX5OPQWWYQ5N7VUAJQL/action/storage_attestation","attest_author":"https://pith.science/pith/RTYYYVNMX5OPQWWYQ5N7VUAJQL/action/author_attestation","sign_citation":"https://pith.science/pith/RTYYYVNMX5OPQWWYQ5N7VUAJQL/action/citation_signature","submit_replication":"https://pith.science/pith/RTYYYVNMX5OPQWWYQ5N7VUAJQL/action/replication_record"}},"created_at":"2026-07-04T15:55:50.290307+00:00","updated_at":"2026-07-04T15:55:50.290307+00:00"}